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| /*===================================================================*/
/* NRDF D0390 Data No.24 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,24;
D#=D1434;
TITLE=/Nuclear structure of even lead isotopes by the (p,t) reaction/;
ATH=(M.TAKAHASHI'1', T.MURAKAMI'1', S.MORITA'1', H.ORIHARA'2',
Y.ISHIZAKI'3', H.YAMAGUCHI'4');
INST-ATH=(2JPNTOH'1', 2JPNTOH'2', 2JPNINS'3', 2JPNTKS'4');
/* '1' Department of Physics */
/* '2' Cyclotron and Radioisotope Center */
/* '3' Institute for Nuclear Study */
/* '4' Faculty of General Education */
REF=PR/C;
VLP=27(1983)1454;
RCTS=(208PB(P,T)206PB, 206PB(P,T)204PB, 204PB(P,T)202PB);
PHQS=ANGL-DSTRN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,24;
/* 2003-10-24 : Converted, Data converted to EXFOR E1434 and EXFOR
O0685 */
PHQ=ANGL-DSTRN;
ENR=>99%;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYNCYC;
INST-ACC=2JPNINS;
INC-ENGY-LAB=51.9MEV;
POL-PRJ=0%;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'5',PROP-CNTR'6',SCT);
/* '5' To analyze triton momentum */
/* '6' Array of 200 proportional counters serve as position
detectors. They form counter telescopes in combination with
scintillation counters. */
ERS-DET=[90KEV'7';
/* '7' Overall energy resolution for the tritons of interest */
ANL=DWBA'8';
/* '8' Zero-range DWBA approximation (code DWUCK-4, [W.A.Lanford
and J.B.McGrory, Michigan State University Cyclotron Laboratory
Report No.MSUCL-81, 1973 (unpublished); Phys. Lett.
45B(1973)283]) */
RCT=206PB(P,T)204PB;
CHM=ELM;
PHYS-FORM=SLD'114';
/* '114' Metallic foil */
THK-TGT=5MG/CM**2;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,24;
INC-ENGY-LAB=51.9MEV;
SYS-ERR=<20%'115';
/* '115' Error of the absolute cross section of the ground state
transition is estimated to be less than 20%, where the main
part comes from the uncertainty of the solid angle of each
counter on the focal plane of the magnetic spectrograph. */
EMT=T;
RSD=204PB;
EXC-ENGY=1.80MEV;
J-PTY=4+;
DELTA-THTC=0.25DEG'116';
/* '116' Data-point reader uncertainty */
DELTA-DSIGMA/DOMEGA=1.9%'117';
/* '117' Data-point reader uncertainty */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'118'
(DEG) (UB/SR) (%)
4.77 76.1 +-X
7.56 57.5 +-X
9.36 43.4 +-X
11.75 38.6 +-X
14.54 37. +-X
17.13 33.3 +-X
20.12 26.7 +-X
22.31 24.5 +-X
24.9 21.1 +-X
27.69 22.4 +-X
32.68 12.62 +-X
37.27 8.23 +-X
40.45 9. +-X
42.84 8.49 +-X
47.82 6.23 +-X
53.01 3.61 +-X
57.98 3.31 +-7.
62.78 1.83 +-15.
INC-ENGY-LAB=42MEV;
CMPD=40CA;
RSD=39K;
EXC-ENGY-CMPD=11.98MEV;
J-PTY-CMPD=0+;
ISOSPIN-CMPD=2;
EXC-ENGY=0MEV;
THTL=27DEG;
/*@5@*/
/*FIG.20-(2)*/
/* D390 FIG.20-(2) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
CHANNEL'1' COUNT'2' DELTA-COUNT
(NODIM) (NODIM) (NODIM)
10.928 5.855E+00 +-XXXXXXXXX
11.919 6.045E+00 +-XXXXXXXXX
12.913 6.505E+00 +-XXXXXXXXX
13.894 5.344E+00 +-XXXXXXXXX
14.952 3.367E+00 +-XXXXXXXXX
15.859 3.293E+00 +-XXXXXXXXX
16.937 4.017E+00 +-XXXXXXXXX
17.929 4.206E+00 +-XXXXXXXXX
18.928 5.477E+00 +-XXXXXXXXX
19.745 4.329E+00 +-XXXXXXXXX
20.817 4.243E+00 +-XXXXXXXXX
21.967 3.609E+00 +-XXXXXXXXX
22.888 5.426E+00 +-0.189E+01
24.033 3.982E+00 +-0.108E+01
24.972 8.230E+00 +-0.162E+01
25.931 4.098E+00 +-0.162E+01
27.007 4.551E+00 +-0.162E+01
27.995 4.201E+00 +-0.810E+00
28.980 3.581E+00 +-0.135E+01
30.072 6.195E+00 +-0.216E+01
31.099 1.658E-01 +-0.406E+01
32.012 1.171E+01 +-0.621E+01
33.138 7.838E+00 +-0.514E+01
34.030 5.874E+00 +-0.486E+01
35.018 5.523E+00 +-0.324E+01
35.993 3.553E+00 +-0.378E+01
37.075 4.816E+00 +-0.217E+01
38.089 7.977E+00 +-0.162E+01
39.077 7.627E+00 +-0.136E+01
40.192 2.401E+00 +-XXXXXXXXX
41.027 3.685E+00 +-XXXXXXXXX
42.212 7.643E+00 +-XXXXXXXXX
43.171 3.511E+00 +-XXXXXXXXX
44.183 6.402E+00 +-XXXXXXXXX
45.156 4.161E+00 +-XXXXXXXXX
46.090 7.599E+00 +-XXXXXXXXX
47.166 8.052E+00 +-XXXXXXXXX
48.248 9.315E+00 +-XXXXXXXXX
49.064 8.168E+00 +-XXXXXXXXX
50.146 9.432E+00 +-XXXXXXXXX
51.091 3.410E+00 +-XXXXXXXXX
52.093 4.950E+00 +-XXXXXXXXX
53.012 6.497E+00 +-XXXXXXXXX
54.096 8.031E+00 +-XXXXXXXXX
55.162 7.133E+00 +-XXXXXXXXX
56.143 5.973E+00 +-XXXXXXXXX
57.232 8.047E+00 +-XXXXXXXXX
57.955 5.556E+00 +-XXXXXXXXX
59.124 7.353E+00 +-XXXXXXXXX
60.019 5.659E+00 +-XXXXXXXXX
\END;
/*===================================================================*/
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